{"title":"A Case Study on using CPML and PML Boundary Conditions in FDTD for RCS Calculation","authors":"N. K. Sahoo, R. K. Parida, D. C. Panda","doi":"10.1109/AESPC44649.2018.9033411","DOIUrl":null,"url":null,"abstract":"Perfect Matched Layer (PML) and Convolutional PML boundary conditions are used in FDTD for Radar Cross Section (RCS) calculation of a perfect electric conducting (PEC) sphere. Matlab is used for coding the FDTD. The results obtained are compared with that of results obtained using FEKO full-wave electromagnetic simulation software. It is seen that the CPML boundary condition takes less simulation time with the smaller computational domain without compromising accuracy.","PeriodicalId":222759,"journal":{"name":"2018 International Conference on Applied Electromagnetics, Signal Processing and Communication (AESPC)","volume":"72 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 International Conference on Applied Electromagnetics, Signal Processing and Communication (AESPC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/AESPC44649.2018.9033411","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Perfect Matched Layer (PML) and Convolutional PML boundary conditions are used in FDTD for Radar Cross Section (RCS) calculation of a perfect electric conducting (PEC) sphere. Matlab is used for coding the FDTD. The results obtained are compared with that of results obtained using FEKO full-wave electromagnetic simulation software. It is seen that the CPML boundary condition takes less simulation time with the smaller computational domain without compromising accuracy.